colloids
colloidal color
Gold, copper, or silver nanoparticles grown inside the glass absorb light by plasmon resonance — the deep reds of gold ruby and cranberry glass. The color isn't there until a controlled reheat strikes it.
Colloidal color in glass works by growing metal nanoparticles — gold, copper, or silver — inside the glass after it is formed, then letting those particles absorb light. The mechanism is physically distinct from dissolved-ion color: here the absorbing entity is a metallic particle tens of nanometers across, not a single ion. The phenomenon is called surface plasmon resonance, and it produces colors of an intensity and depth that dissolved ions cannot match: the deep red of gold ruby, the warm crimson of copper ruby, the yellow of silver stain.
The mechanism’s signature feature is that the color does not exist when the glass leaves the furnace. A gold ruby gather fresh from the melt is colorless or faintly tinted. The color appears only during a controlled reheat called striking, which nucleates and grows the colloids. A goblet unstruck in storage looks like clear glass; held over a torch for the right amount of time, it blooms red. This delayed appearance — and the skill required to read it — made ruby glass one of the most prized and difficult products of the medieval and Baroque glassmaker’s repertoire.
How it works
When a metal nanoparticle much smaller than the wavelength of light sits inside a transparent glass, the particle’s conduction electrons behave like a cloud in a box: an incoming light wave drives them into collective oscillation. At the resonance frequency, the particle absorbs light ferociously — far more strongly per atom than any dissolved ion. For gold spheres roughly 5–60 nm across in silicate glass, the resonance sits near 530 nm (green): green is absorbed, and the transmitted remainder is the ruby red that has made gold glass famous for two thousand years.
Particle size tunes the color. As gold particles grow coarser during striking, the resonance shifts and broadens. A perfectly struck ruby is clear red; over-striking pushes it toward purple, then a muddy blue-gray — what glassmakers call livered glass. The craftsman’s failure mode is a nanoscale geometry error made visible by eye.
Silver resonates at shorter wavelengths, near 410–450 nm (blue absorbed, yellow transmitted), which is why silver in glass gives yellow rather than red. Copper’s resonance sits near 565 nm with additional interband absorption, producing a deep oxblood red similar to gold’s but achievable at far lower cost.
Striking. The metal enters the melt in ionic form — gold dissolved via aqua regia, copper as an oxide — accompanied by a reducing agent. Historically, tin was the classic reductant for gold, and the standard gold preparation for ruby glass was Purple of Cassius, a gold-tin co-precipitate described by Andreas Cassius in the 1680s. The Potsdam glassmaker Johann Kunckel turned this chemistry into reliable ruby glass production in the same decade, the culmination of decades of European workshop experimentation.
On the reheat — typically 500–700 °C — reduced metal atoms nucleate and aggregate into colloids. Time and temperature control the particle size, and particle size controls the color. The striking schedule is the recipe.
Artifact stories
Gold ruby
Gold ruby glass contains actual gold — roughly 0.01–0.1% by weight — and this cost means it is often used as flashed glass for sheet and window applications, a thin ruby layer fused over a clear gather. Solid body color is used for vessels and tableware, where the thin walls keep gold content manageable. In the dilute form known as cranberry glass, the gold loading is lower still, producing a warm pink rather than a deep red. Cranberry became a popular Victorian tableware color: the delicate pink reads jewel-like in thin-blown pieces, and the dilution kept costs manageable.
The tradition of ruby glass stretches back to ancient Rome, but Kunckel’s 17th-century Potsdam workshop established the chemical principles that made production reliable. The ware he made — now held in museum collections across Europe — shows the full range from pale cranberry pink to deep garnet, the variation arising from different striking schedules on the same base composition.
Copper ruby follows the same striking logic and is the industrial and historical substitute when gold is too expensive. Medieval reds in stained glass windows are almost always copper ruby, flashed thin over clear glass because a full-thickness copper ruby sheet reads nearly black.
The Lycurgus Cup
The Lycurgus Cup, a Roman cage cup now in the British Museum dated to approximately the 4th century CE, is the canonical demonstration of what nanoparticles in glass can do. The cup contains roughly 70 nm gold-silver alloy particles that both absorb and scatter light.
In reflected light — looking at the cup under normal room lighting — it appears opaque pea-green: scattered light dominates. Lit from behind, it glows translucent wine-red: transmitted light passing through the absorbing colloid reaches the eye. One object, two colors, zero pigment. The effect is pure nanoparticle optics, and the craftsmen who made it had no idea their colorant was metallic particles at all. The composition was not identified until electron microscopy analysis in the 1990s.
The Lycurgus Cup is the standard exhibit-A for ancient accidental nanotechnology, and it demonstrates something worth holding: people can achieve nanoscale precision through empirical craft knowledge centuries before they have the scientific language to describe what they are doing.
Curves are illustrative approximations and the swatch is a coarse RGB rendering, not a full CIE colorimetric pipeline.
A stylized striking timeline — real schedules are composition-specific and the over-struck endpoint is the failure mode, not a destination.
A stylized rendering — the real cup is in the British Museum, and its dichroism comes from gold-silver alloy nanoparticles.